fix doxygen reflinks

diff --git a/include/deal.II/base/function_lib.h b/include/deal.II/base/function_lib.h
index 25bc871c2bf8e0b8b4ba87bbc6e81b86f285a947..3559bb335ad5789ea45516404499e1eaaedabbba 100644 (file)
--- a/include/deal.II/base/function_lib.h
+++ b/include/deal.II/base/function_lib.h
@@ -1774,30 +1774,30 @@ namespace Functions
    * to strong rotation and elongation of the fluid @cite Blais2013.
    *
    * The stream function $\Psi$ of this Rayleigh-Kothe vortex is defined as:
-@f[
-\Psi = \frac{1}{\pi} \sin^2 (\pi x) \sin^2 (\pi y) \cos \left( \pi \frac{t}{T}
-\right)
-@f]
+   * @f[
+   * \Psi = \frac{1}{\pi} \sin^2 (\pi x) \sin^2 (\pi y) \cos \left( \pi
+   * \frac{t}{T} \right)
+   * @f]
    * where $T$ is half the period of the flow. The velocity profile in 2D
-($\textbf{u}=[u,v]^T$) is :
-@f{eqnarray*}{
-   u &=&  - \frac{\partial\Psi}{\partial y} = -2 \sin^2 (\pi x) \sin (\pi y)
-\cos (\pi y)  \cos \left( \pi \frac{t}{T} \right)\\ v &=&
-\frac{\partial\Psi}{\partial x} = 2 \cos(\pi x) \sin(\pi x) \sin^2 (\pi y) \cos
-\left( \pi \frac{t}{T} \right)
-@f}
+   * ($\textbf{u}=[u,v]^T$) is:
+   * @f{eqnarray*}{
+   * u &=&  - \frac{\partial\Psi}{\partial y} = -2 \sin^2 (\pi x) \sin (\pi y)
+   * \cos (\pi y)  \cos \left( \pi \frac{t}{T} \right)\\ v &=&
+   * \frac{\partial\Psi}{\partial x} = 2 \cos(\pi x) \sin(\pi x) \sin^2 (\pi y)
+   * \cos \left( \pi \frac{t}{T} \right)
+   * @f}
    * where $T$ is half the period of the flow.
    *
    * The velocity profile is illustrated in the following animation:
    *
-@htmlonly
-<p align="center">
-  <iframe width="560" height="500"
-src="https://www.youtube.com/embed/m6hQm7etji8" frameborder="0"
-   allow="accelerometer; autoplay; encrypted-media; gyroscope;
-picture-in-picture" allowfullscreen></iframe>
- </p>
-@endhtmlonly
+   * @htmlonly
+   * <p align="center">
+   *   <iframe width="560" height="500"
+   * src="https://www.youtube.com/embed/m6hQm7etji8" frameborder="0"
+   *    allow="accelerometer; autoplay; encrypted-media; gyroscope;
+   * picture-in-picture" allowfullscreen></iframe>
+   *  </p>
+   * @endhtmlonly
    *
    * It can be seen that this velocity reverses periodically due to the term
    * $\cos \left( \pi \frac{t}{T} \right)$ and that material will end up at its

diff --git a/include/deal.II/dofs/dof_tools.h b/include/deal.II/dofs/dof_tools.h
index 7d1d3659453a85d6ea12284d83cdaea9d43215c3..1f3ebcfc138dfb66c7c6af136a4ee2909a0a5b56 100644 (file)
--- a/include/deal.II/dofs/dof_tools.h
+++ b/include/deal.II/dofs/dof_tools.h
@@ -132,8 +132,9 @@ namespace DoFTools
  * With this vector, one can get, for any given degree of freedom, a unique
  * number among those DoFs that sit on the boundary; or, if your DoF was
  * interior to the domain, the result would be numbers::invalid_dof_index. We
- * need this mapping, for example, to build the @ref GlossMassMatrix "mass
- * matrix" on the boundary (for this, see make_boundary_sparsity_pattern()
+ * need this mapping, for example, to build the
+ * @ref GlossMassMatrix "mass matrix"
+ * on the boundary (for this, see make_boundary_sparsity_pattern()
  * function, the corresponding section below, as well as the MatrixCreator
  * namespace documentation).
  *

diff --git a/include/deal.II/fe/fe_hermite.h b/include/deal.II/fe/fe_hermite.h
index 3e3172bdebc47ea6342e4b2c977673731682eef0..d37980e7c262d8cf00811a931118f06a6d059e98 100644 (file)
--- a/include/deal.II/fe/fe_hermite.h
+++ b/include/deal.II/fe/fe_hermite.h
@@ -74,21 +74,21 @@ DEAL_II_NAMESPACE_OPEN
  * <code>FE_Hermite<3>(3)</code>:
  *
  * @verbatim
- *       (40,41,44,45)__(42,43,46,47)          (40,41,44,45)__(42,43,46,47)
- *       (56,57,60,61)  (58,59,62,63)          (56,57,60,61)  (58,59,62,63)
- *          /  |              |                    /           /  |
- *         /   |              |                   /           /   |
- *        /    |              |                  /           /    |
- *(32,33,36,37)|              |         (32,33,36,37)__(34,35,38,39)
- *(48,49,52,53)|              |         (48,49,52,53)  (50,51,54,55)
- *       |     |              |                |            |     |
- *       |( 8,9,12,13 )__(10,11,14,15)         |            |(10,11,14,15)
- *       |(24,25,28,29)  (26,27,30,31)         |            |(26,27,30,31)
- *       |    /              /                 |            |    /
- *       |   /              /                  |            |   /
- *       |  /              /                   |            |  /
- *  (  0,1,4,5  )___(  2,3,6,7  )      (  0,1,4,5  )___(  2,3,6,7  )
- *  (16,17,20,21)   (18,19,22,23)      (16,17,20,21)   (18,19,22,23)
+ *        (40,41,44,45)__(42,43,46,47)          (40,41,44,45)__(42,43,46,47)
+ *        (56,57,60,61)  (58,59,62,63)          (56,57,60,61)  (58,59,62,63)
+ *           /  |              |                    /           /  |
+ *          /   |              |                   /           /   |
+ *         /    |              |                  /           /    |
+ * (32,33,36,37)|              |         (32,33,36,37)__(34,35,38,39)
+ * (48,49,52,53)|              |         (48,49,52,53)  (50,51,54,55)
+ *        |     |              |                |            |     |
+ *        |( 8,9,12,13 )__(10,11,14,15)         |            |(10,11,14,15)
+ *        |(24,25,28,29)  (26,27,30,31)         |            |(26,27,30,31)
+ *        |    /              /                 |            |    /
+ *        |   /              /                  |            |   /
+ *        |  /              /                   |            |  /
+ *   (  0,1,4,5  )___(  2,3,6,7  )      (  0,1,4,5  )___(  2,3,6,7  )
+ *   (16,17,20,21)   (18,19,22,23)      (16,17,20,21)   (18,19,22,23)
  * @endverbatim
  *
  * Due to the increased regularity constraints many of these functions are

diff --git a/include/deal.II/lac/cuda_solver_direct.h b/include/deal.II/lac/cuda_solver_direct.h
index 33e3aa83d43d5a88fd5188f6c1d9753cefc3d337..604cff147e41d059817f73ead28319c69a5e3629 100644 (file)
--- a/include/deal.II/lac/cuda_solver_direct.h
+++ b/include/deal.II/lac/cuda_solver_direct.h
@@ -53,7 +53,8 @@ namespace CUDAWrappers
       /**
        * Set the solver type. Possibilities are:
        * <ul>
-       * <li> "Cholesky" which performs a Cholesky decomposition on the @ref GlossDevice "device"
+       * <li> "Cholesky" which performs a Cholesky decomposition on the
+       * @ref GlossDevice "device"
        * </li>
        * <li> "LU_dense" which converts the sparse matrix to a dense
        * matrix and uses LU factorization </li>

diff --git a/include/deal.II/matrix_free/fe_remote_evaluation.h b/include/deal.II/matrix_free/fe_remote_evaluation.h
index 6546a9825afd9775c2d72cef68a5af31b6e28756..a556949b2b6800750ae170a83a7de7ae9575a445 100644 (file)
--- a/include/deal.II/matrix_free/fe_remote_evaluation.h
+++ b/include/deal.II/matrix_free/fe_remote_evaluation.h
@@ -573,17 +573,17 @@ public:
 
   /**
    * @c FERemoteEvaluation does not provide the functions `get_value()` and
-   *`get_gradient()`. To access values and/or gradients call @c
-   *get_data_accessor() on every thread, e.g., `auto remote_evaluator =
-   *get_data_accessor();` The returned object can be used as follows.
-   *@code
+   * `get_gradient()`. To access values and/or gradients call @c
+   * get_data_accessor() on every thread, e.g., `auto remote_evaluator =
+   * get_data_accessor();` The returned object can be used as follows.
+   * @code
    * for (unsigned int entity = range.first; entity < range.second; ++entity)
    * {
    *    remote_evaluator.reinit(entity);
    *    for(unsigned int q : quadrature_point_indices())
    *      remote_evaluator.get_value(q)
    * }
-   *@endcode
+   * @endcode
    */
   internal::PrecomputedEvaluationDataAccessor<dim, n_components, value_type>
   get_data_accessor() const;